RESUMO
Thermal management is an important consideration for most nanoelectronic devices, and an understanding of the thermal conductivity of individual device components is critical for the design of thermally efficient systems. However, it can be difficult to directly probe local changes in thermal conductivity within a nanoscale system. Here, we utilize the time-resolved and diffraction-limited imaging capabilities of ultrafast pump-probe microscopy to determine, in a contact-free configuration, the local thermal conductivity in individual Si nanowires (NWs). By suspending single NWs across microfabricated trenches in a quartz substrate, the properties of the same NW both on and off the substrate are directly compared. We find the substrate has no effect on the recombination lifetime or diffusion length of photogenerated charge carriers; however, it significantly impacts the thermal relaxation properties of the NW. In substrate-supported regions, thermal energy deposited into the lattice by the ultrafast laser pulse dissipates within â¼10 ns through thermal diffusion and coupling to the substrate. In suspended regions, the thermal energy persists for over 100 ns, and we directly image the time-resolved spatial motion of the thermal signal. Quantitative analysis of the transient images permits direct determination of the NW's local thermal conductivity, which we find to be a factor of â¼4 smaller than in bulk Si. Our results point to the strong potential of pump-probe microscopy to be used as an all-optical method to quantify the effects of localized environment and morphology on the thermal transport characteristics of individual nanostructured components.
RESUMO
Crystal structures have been determined for the three-member set of cofacial silicon phthalocyanines, ((n-C(6)H(13))(3)SiO)[SiPcO](1-3)(Si(n-C(6)H(13))(3)). The staggering angles between adjacent rings in the dimer and trimer of this set are â¼16°. The interactions leading to these angles have been investigated by the atoms-in-molecules (AIM) and reduced-density-gradient (RDG) methods. The results show that long directional interactions (LDIs) are responsible for these angles. A survey of the staggering angles in various cofacial phthalocyanines described in the literature has revealed the existence of significant LDIs in a number of them. It is apparent that in many cases the ability of LDIs to dominate the forces giving rise to the staggering angles observed in cofacial phthalocyanines depends on their inter-ring separations.